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Measurement of WW Production with the ATLAS detector at  s = 8 TeV

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Measurement of WW Production with the ATLAS detector at s = 8 TeV

Kristin Lohwasser On behalf of the ATLAS collaboration

Theory

Event Selection Backgrounds Results

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Measurements of WW Production

Proves non-Abelian structure of electroweak interaction

→ ZWW vertex fixes unitarity problem

Important test of the Standard Model

Sensitive to new physics due to triple gauge couplings

Previous measurement from LHC showed slight

enhancement of data over theoretical predictions

Theoretical background and motivation

1.4 1 1.7

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Theoretical Predictions

MCFM NLO

contains triple gauge coupling

(enhanced cross section for high pT and new physics)

~91% ~2% ~7%

MCFM LO CT10 large k-factor?

NNLO MSTW2008 LHC Higgs XS WS

arXiv:1307.1347

Contributions neglected in this SM prediction

qq → WW (NLO → NNLO+NNLL k-factor) + 1.6 pb

gg → WW (LO → NNLO+NNLL k-factor) + 1.4 up to +2.8 pb

Electroweak corrections – 0.5 pb

γγ-induced WW + 0.5 pb

Vector boson scattering + 0.5 pb

Double parton interaction + 0.04 pb

Theoretical background and motivation

Total sum of:

+ 3.5 to 4.9 pb

Interference neglected

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ATLAS Detector

Event Selection

muons and electrons

identified and well-isolated di- and single lepton trigger

pT>20 and 25 GeV

(subleading, leading)

Missing energy

vectorial sum of

calorimeter deposits

ETMiss,rel>45 GeV (ee,μμ) ETMiss,rel >15 GeV (eμ)

ETMiss,rel = ETMiss sin(ETMiss – jets,lep (if else ETMiss,rel = ETMiss)

Data taken at

s = 8 TeV

integrated luminosity

∫ L dt = 20.3 fb-1 4π-general purpose

detector

excellent particle ID and missing ET

performance

Missing momentum

vectorial sum of tracks pileup-robust

pTMiss> 45 and 20 GeV Δφ(pTMiss,ETMiss) <0.3/0.6

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Event Selection

Opposite sign requirement for leptons, outside Z mass window

Top background dominates, rejected by Jet Veto requirement

No jets with pT>25 GeV within ||<4.5

Data driven determination of Z, top and W+jets events

eμ ee+μμ

Event Selection Event Selection

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Data-driven Backgrounds

Top background (12 – 14 %):

Jet veto efficiency applied to MC events to obtain normalization determined from a data control sample of top events with large scalar sum of lepton and jet pT

W+jets background (eμ 4% / ee+μμ 1%):

extract normalization and shape

efficiencies for fake and real leptons for loose and tight cuts

determine signal and background components with matrix method

Z+jets background (eμ 0.3% / ee+μμ 1%):

fit to data control region to extract normalization

Backgrounds

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Backgrounds from Dibosons

Diboson background determined using MC simulation WZ, ZZ, W and W*

Validation region of same sign events with large W+jets contribution

eμ eμ

Missing ET Invariant dilepton mass m(ll)

Backgrounds

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Distributions

6636 WW candidate events observed after full selection (5067 eμ, 594 ee, 975 μμ)

WW MC signal scaled to measured cross sections

Shapes well described

eμ eμ

scaled

scaled scaled

Results

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Extraction of the cross section

Acceptance ee: 0.03 correction μμ: 0.04 eμ: 0.11

Branching ratio (0.108) (0.108) Total

Cross section

ETMiss reconstruction (2-4%)

Background (3-6 %)

Jet energy (2%)

Jet-veto requirement (4-5%)

Luminosity (2.5%)

Total: ~7.5%

Combination of channels performed using likelihood fit

Results

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Combination

Good agreement between the channels

eμ dominates due to smaller uncertainty and larger statistics

Results

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Results

Some variations observed for different PDF predictions

Global data CT10 PDF chosen for its generally good agreement with other LHC data

PDF using LHC + HERA data only gives better agreement

Results

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Conclusion

WW cross section measured at s = 8 TeV using 20.3 fb-1

Robust measurement with data-driven background estimations

Result somewhat higher than prediction

Some contributions neglected: Missing higher order corrections Could amount to several pb

Results public under ATLAS-CONF-2014-033

http://cds.cern.ch/record/1728248

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Thank you!

Referencias

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